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Isotopes of Lawrencium

List, data and properties of all known isotopes of Lawrencium.


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Lawrencium isotopes

Lawrencium is an exclusively artificially produced radioactive chemical element that is not known in nature.

With 258Lr, the first lawrencium isotope was discovered in 1961 by the research team led by Albert Ghiorso at the Lawrence Berkeley National Laboratory University of California.

To date, a total of 11 different isotopes have been produced, all of which are extremely short-lived; with a half-life of about 4 hours, Lawrencium-262 is the most stable Lr nuclide. It is expected that heavier lawrencium nuclides may have longer half-lives.

Atoms or atomic nuclei are generally referred to as lawrencium isotopes or lawrencium nuclides, which have element-specific 103 protons and differ in the number of neutrons in the nucleus.

 

Isotope Table: Lawrencium

The two following tables list the most important data and properties of the Lawrencium isotopes. Further information on the individual Lawrencium isotopes is listed on separate pages and can be accessed via the link in column 1.

 

Atomic Properties

Isotope
Nuclide
ENAtomic Mass
[Nuclear Mass]
{Mass Excess}
Spin I
(h/2π)
Parent
123456
Lawrencium-251251103Lr148251 u
[250.943505 u]
{0 MeV}
Lawrencium-252252103Lr149252.09526(25) u
[252.038765 u]
{88.73412 MeV}
256Db
Lawrencium-253253103Lr150253.09509(22) u
[253.038595 u]
{88.57576 MeV}
(7/2-)257Db
Lawrencium-253m253m103Lr150253.09509(22) u
[253.038595 u]
{88.57576 MeV}
(1/2-)
Lawrencium-254254103Lr151254.09648(32) u
[254.039985 u]
{89.87054 MeV}
258Db
Lawrencium-255255103Lr152255.096562(19) u
[255.040067 u]
{89.94692 MeV}
(1/2-)
Lawrencium-255m1255m1103Lr152255.096562(19) u
[255.040067 u]
{89.94692 MeV}
(7/2-)
Lawrencium-256256103Lr153256.09849(9) u
[256.041995 u]
{91.74284 MeV}
260Db
Lawrencium-257257103Lr154257.09948(5) u
[257.042985 u]
{92.66502 MeV}
9/2+261Db
Lawrencium-258258103Lr155258.10175(11) u
[258.045255 u]
{94.77951 MeV}
262Db
Lawrencium-259259103Lr156259.10290(8) u
[259.046405 u]
{95.85073 MeV}
(9/2+)263Db
Lawrencium-260260103Lr157260.10550(13) u
[260.049005 u]
{98.27262 MeV}
Lawrencium-261261103Lr158261.10688(21) u
[261.050385 u]
{99.55808 MeV}
Lawrencium-262262103Lr159262.10961(21) u
[262.053115 u]
{102.10106 MeV}
Lawrencium-263263103Lr160
Lawrencium-264264103Lr161264.11420(47) u
[264.057705 u]
{106.37661 MeV}
Lawrencium-265265103Lr162
Lawrencium-266266103Lr163266.11983(63) u
[266.063335 u]
{111.62093 MeV}

 

Radioactive Decay Properties

IsotopeRadioactive DecayExtern
Half-lifeDecay ModeProbabilityEnergy
789101112
Lr-251α 247Md
ε ?


AL
Lr-2520.36 sEC/β+252No
α → 248Md
SF div.
?
?
?
5.87(24) MeV
9.164(17) MeV
AL
Lr-2530.57 sα → 249Md
SF div.
98.7 %
1.3 %
8.918(20) MeV
AL
Lr-253m1.49 sα → 249Md
SF div.
92(5) %
8(5) %

AL
Lr-25418.1(18) sEC/β+254No
α → 250Md
SF div.
28.3(19) %
71.7(19) %
< 0.1 %
5.15(30) MeV
8.816(12) MeV
AL
Lr-25531.1(11) sα → 251Md
EC → 255No
SF div.
99.7(1) %
< 0.3(1) %
< 0.1 %
8.556(7) MeV
3.140(23) MeV
AL
Lr-255m12.54(5) sIso → 255Lr
α → 251Md
ca. 60 %
ca. 40 %

Lr-25627.9 sEC/β+256No
α → 253Md
SF div.
15(10) %
85(10) %
< 0.03 %
3.92(8) MeV
8.81(10) MeV
AL
Lr-2574 sα → 253Md
EC → 257No
SF div.
< 100 %
< 15 %
< 0.033 %
9.07(3) MeV
2.42(4) MeV
AL
Lr-2583.92(33) sα → 254Md
EC → 258No
97.4(18) %
2.6 (18)
8.904(19) MeV
3.30(14) MeV
AL
Lr-2596.2(3) sα → 255Md
SF div.
78(2) %
22(2) %
8.58(7)
AL
Lr-260180(30) sα → 256Md
EC → 260No
80(20) %
< 40 %
8.40(14) MeV
2.66(24) MeV
AL
Lr-26139(12) minSF div.?AL
Lr-2624 hSF div.
EC/β+262No
α → 258Md
< 10 %
?
?

2.00(41) MeV
7.99(20) MeV
AL
Lr-263gibt es nichtAL
Lr-2644.9 hSF divca. 100 %AL
Lr-265unknownAL
Lr-26611 hSF div.100 %AL

 

Notes (related to the columns):

1 - name of the nuclide, isotope.
2 - E: isotope symbol with mass number (superscript; number of nucleons) and Atomic number (subscript; number of protons).
3 - N: number of neutrons.
4 - relative atomic mass of the Lawrencium isotope (isotopic mass including electrons) and the mass of the atomic nucleus in square brackets (nuclear mass, nuclide mass without electrons), each related to 12C = 12.00000 [2]. In addition, the mass excess is given in MeV.
5 - nuclear spin I, unit: h/2π.
6 - source nuclides: Possible, assumed or actual source nuclides (mother nuclides, parent nuclides). If applicable, the corresponding decay modes can be found in the data for the respective starting nuclide.

7 - isotope notation in short form.
8 - decay: half-live of the Lawrencium isotope (a = years; ; d = days; h = hours; min = minutes; s = seconds).
9 - decay mode: type of decay into the respective daughter nuclides with n = neutron emission; p = proton emission; α = alpha decay; β- = beta minus decay with electron emission; EC = electron capture; β+ = positron emission; ε = β+ and/or EC; Iso = isomeric transition; CD = cluster decay; SF = spontaneous decay.
10 - decay probability in percent (%).
11 - decay energy; Particle energy related to decay type.
12 - other information and notes: AL = Adopted Levels (link to external data [1]).

Miscellaneous:

()- Numbers in brackets: uncertainty to represent the spread of the reported value.
~ - Theoretical values or systematic trends.
  - unlisted-: Nuclides that have already been mentioned in the literature but for some reason can no longer be found in the current nuclide tables because their discovery e.g. has not confirmed.

 

Literature Sources and References

Properties of the Lawrencium nucleides

[1] - NuDat: National Nuclear Data Center, Brookhaven National Laboratory, based on ENSDF and the Nuclear Wallet Cards.

[2] - G. Audi et. al.: The NUBASE evaluation of nuclear and decay properties. Nuclear Physics, (2003), DOI 10.1016/j.nuclphysa.2003.11.001.

[3] - Live Chart of Nuclides. Nuclear structure and decay data.

Lawrencium: NMR properties

[4] - N. J. Stone: Table of nuclear magnetic dipole and electric quadrupole moments. Atomic Data and Nuclear Data Tables, (2005), DOI 10.1016/j.adt.2005.04.001.

[5] - Pekka Pyykkö: Year-2008 nuclear quadrupole moments. Molecular Physics, (2008), DOI 10.1080/00268970802018367.

[6] - Pekka Pyykkö: Year-2017 nuclear quadrupole moments. Molecular Physics, (2018), DOI 10.1080/00268976.2018.1426131.

[7] - N. J. Stone: Table of recommended nuclear magnetic dipole moments. IAEA, (2019).

More sources:

[8] - Isotopic abundances, atomic weights and isotopic masses: see respective keyword.

[9] - J. Khuyagbaatar et al.:
48Ca + 249Bk Fusion Reaction Leading to Element Z = 117: Long-Lived α-Decaying 270Db and Discovery of 266Lr.
In: Physical Review Letters, (2014), DOI 10.1103/PhysRevLett.112.172501.

 


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Last update: 2022-11-30


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